An Oceanic General Circulation Model (OGCM) investigation of the Red Sea circulation: 2. Three‐dimensional circulation in the Red Sea

[1] The three-dimensional circulation of the Red Sea is studied using a set of Miami Isopycnic Coordinate Ocean Model (MICOM) simulations. The model performance is tested against the few available observations in the basin and shows generally good agreement with the main observed features of the circulation. The main findings of this analysis include an intensification of the along-axis flow toward the coasts, with a transition from western intensified boundary flow in the south to eastern intensified flow in the north, and a series of strong seasonal or permanent eddy-like features. Model experiments conducted with different forcing fields (wind-stress forcing only, surface buoyancy forcing only, or both forcings combined) showed that the circulation produced by the buoyancy forcing is stronger overall and dominates the wind-driven part of the circulation. The main circulation pattern is related to the seasonal buoyancy flux (mostly due to the evaporation), which causes the density to increase northward in the basin and produces a northward surface pressure gradient associated with the downward sloping of the sea surface. The response of the eastern boundary to the associated mean crossbasin geostrophic current depends on the stratification and b-effect. In the northern part of the basin this results in an eastward intensification of the northward surface flow associated with the presence of Kelvin waves while in the south the traditional westward intensification due to Rossby waves takes place. The most prominent gyre circulation pattern occurs in the north where a permanent cyclonic gyre is present that is involved in the formation of Red Sea Outflow Water (RSOW). Beneath the surface boundary currents are similarly intensified southward undercurrents that carry the RSOW to the sill to flow out of the basin into the Indian Ocean. INDEX TERMS: 4243 Oceanography: General: Marginal and semienclosed seas; 4255 Oceanography: General: Numerical modeling; 4532 Oceanography: Physical: General circulation; KEYWORDS: Red Sea, marginal sea, Oceanic General Circulation Model, water mass formation

[1]  Rainer Bleck,et al.  Salinity-driven Thermocline Transients in a Wind- and Thermohaline-forced Isopycnic Coordinate Model of the North Atlantic , 1992 .

[2]  C. Garrett,et al.  The Heat and Freshwater Budgets of the Red Sea , 1999 .

[3]  W. Johns,et al.  An Oceanic General Circulation Model (OGCM) investigation of the Red Sea circulation, 1. Exchange between the Red Sea and the Indian Ocean , 2002 .

[4]  F. Schott,et al.  Hydrographic Structure of the Convection Regime in the Gulf of Lions: Winter 1987 , 1991 .

[5]  C. Garrett,et al.  The shallow thermohaline circulation of the Red Sea , 1997 .

[6]  S. A. Morcos,et al.  Physical and chemical oceanography of the Red Sea , 1970 .

[7]  J. McCreary,et al.  Thermohaline forcing of eastern boundary currents : With application to the circulation off the west coast of Australia , 1986 .

[8]  S. Levitus Climatological Atlas of the World Ocean , 1982 .

[9]  H. Stommel A survey of ocean current theory , 1957 .

[10]  W. Patzert Wind-induced reversal in Red Sea circulation☆ , 1974 .

[11]  N. Hogg The preconditioning phase of MEDOC 1969—II. Topographic effects , 1973 .

[12]  J. Fischer,et al.  Preconditioning the Greenland Sea for deep convection: Ice formation and ice drift , 1995 .

[13]  O. Phillips On turbulent convection currents and the circulation of the Red Sea , 1966 .

[14]  Detlef Quadfasel,et al.  Gyre-scale circulation cells in the Red Sea , 1993 .

[15]  E. Degens,et al.  Hot Brines and Recent Heavy Metal Deposits in the Red Sea , 1969 .

[16]  D. Privett Monthly charts of evaporation from the N. Indian Ocean (including the Red Sea and the Persian Gulf) , 1959 .

[17]  G. Siedler Schichtungs- und Bewegungsverhältnisse am Südausgang des Roten Meeres , 1965 .

[18]  W. Johns,et al.  Heat and freshwater budgets in the Red Sea from direct observations at Bab el Mandeb , 2002 .

[19]  E. Tragou,et al.  A mixed-layer study of the formation of Levantine Intermediate Water , 1993 .

[20]  G. Siedler General Circulation of Water Masses in the Red Sea , 1969 .

[21]  K. Alverson Topographic preconditioning of open ocean deep convection , 1995 .

[22]  D. Quadfasel,et al.  Renewal of deep water in the Red Sea during 1982–1987 , 1996 .

[23]  A. Lascaratos Estimation of deep and intermediate water mass formation rates in the Mediterranean Sea , 1993 .

[24]  J. Swallow,et al.  The preconditioning phase of MEDOC 1969—I. Observations , 1973 .

[25]  Arnold L. Gordon,et al.  Deep Antarctic Convection West of Maud Rise , 1978 .

[26]  W. Johns,et al.  Direct observations of seasonal exchange through the Bab el Mandab Strait , 1997 .

[27]  G. R. Goldsbrough Ocean Currents Produced by Evaporation and Precipitation , 1933 .

[28]  Martin Visbeck,et al.  OBSERVATIONS OF VERTICAL CURRENTS AND CONVECTION IN THE CENTRAL GREENLAND SEA DURING THE WINTER OF 1988-1989 , 1993 .

[29]  M. Maury,et al.  The Physical Geography of the Sea, and Its Meteorology , 1861 .

[30]  R. Muench Relict Convective Features in the Weddell Sea , 1991 .

[31]  C. Maillard,et al.  and exchanges with the Indian Ocean In summer , 1986 .

[32]  H. Stommel The delicate interplay between wind-stress and buoyancy input in ocean circulation: the Goldsbrough variations* , 1984 .

[33]  W. Johns,et al.  Wind induced sea level variability in the Red Sea , 2001 .

[34]  R. Clarke,et al.  The Formation of Labrador Sea Water. Part I: Large-Scale Processes , 1983 .

[35]  R. P. Cember On the sources, formation, and circulation of Red Sea deep water , 1988 .

[36]  A. Neumann,et al.  Circulation of the Red Sea in early summer , 1961 .

[37]  Lakshmi Kantha,et al.  An oceanographic nowcast/forecast system for the Red Sea , 1997 .